Mathematics Objective Questions and Answers: Vector Algebra
Access targeted multiple-choice questions for Vector Algebra designed to align with the latest JEE academic syllabus for JEE Mathematics. These objective practice sets help students evaluate their conceptual understanding and improve exam readiness.
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Multiple Choice Questions
(a) \( 2\hat{i}−6\hat{j}+2\hat{k} \)
(b) \( 6\hat{i}−2\hat{j}+6\hat{k} \)
(c) \( −6\hat{i}+2\hat{j}−6\hat{k} \)
(d) \( 6\hat{i}+2\hat{j}+6\hat{k} \)
Show Answer & Explanation
Answer: (b) \( 6\hat{i}−2\hat{j}+6\hat{k} \)
Explanation:
1. \( \vec{a}×\vec{b}=\begin{vmatrix}\hat{i}&\hat{j}&\hat{k}\\1&1&1\\1&-1&1\end{vmatrix}=2\hat{i}−2\hat{k} \).
2. \( (\vec{a}×\vec{b})×\vec{c}=(2,0,−2)×(2,3,−1)=(0·(−1)−(−2)·3,\ (−2)·2−2·(−1),\ 2·3−0)=(6,−2,6) \).
3. So the result is \( 6\hat{i}−2\hat{j}+6\hat{k} \).
Teacher's Note:
1. Always compute the inner cross product first and keep the order of the factors.
2. Swapping the order of a cross product changes the sign.
(a) 1
(b) 0
(c) −1
(d) 2
Show Answer & Explanation
Answer: (b) 0
Explanation:
1. \( (\vec{a}×\vec{b})×\vec{c}=(\vec{a}·\vec{c})\vec{b}−(\vec{b}·\vec{c})\vec{a} \).
2. \( \vec{a}·\vec{c}=1 \) and \( \vec{b}·\vec{c}=1 \), so \( (\vec{a}×\vec{b})×\vec{c}=\vec{b}−\vec{a} \).
3. Hence \( λ=−1, μ=1 \) and \( λ+μ=0 \).
Teacher's Note:
1. Use the identity for the vector triple product (middle vector times dot product with the third, minus the first times dot product of the other two).
2. Then compare coefficients of the independent vectors.
(a) \( \sqrt{10} \)
(b) 1
(c) 2
(d) \( \sqrt5 \)
Show Answer & Explanation
Answer: (d) \( \sqrt5 \)
Explanation:
1. \( \vec{a}·\vec{c}=8+6−12=2 \) and \( \vec{a}·\vec{b}=2+3−4=1 \).
2. \( \vec{a}×(\vec{b}×\vec{c})=2\vec{b}−1·\vec{c}=(2−4,\ 2−2,\ 2−3)=(−2,0,−1) \).
3. Its magnitude is \( \sqrt{4+0+1}=\sqrt5 \).
Teacher's Note:
1. Evaluating the two dot products first is much shorter than finding two cross products.
2. Check the final magnitude with the Pythagoras formula.
(a) The scalar 0
(b) The null vector \( \vec0 \)
(c) The scalar 1
(d) \( (\vec{a}×\vec{b})·\vec{c} \)
Show Answer & Explanation
Answer: (b) The null vector \( \vec0 \)
Explanation:
1. Expand each term: \( (\vec{a}·\vec{c})\vec{b}−(\vec{a}·\vec{b})\vec{c} \), \( (\vec{b}·\vec{a})\vec{c}−(\vec{b}·\vec{c})\vec{a} \) and \( (\vec{c}·\vec{b})\vec{a}−(\vec{c}·\vec{a})\vec{b} \).
2. Adding, every term cancels in pairs.
3. The result is the null vector (the Jacobi identity).
Teacher's Note:
1. The result is a vector, so it is the null vector, not the scalar zero.
2. This identity is used to simplify sums of cyclic triple products.
(a) \( (\vec{a}×\vec{c})×\vec{b}=\vec0 \)
(b) \( \vec{a}×(\vec{c}×\vec{b})=\vec0 \)
(c) \( \vec{c}×(\vec{b}×\vec{a})=\vec0 \)
(d) \( [\vec{a}\ \vec{b}\ \vec{c}]=1 \)
Show Answer & Explanation
Answer: (a) \( (\vec{a}×\vec{c})×\vec{b}=\vec0 \)
Explanation:
1. \( (\vec{a}×\vec{b})×\vec{c}=(\vec{a}·\vec{c})\vec{b}−(\vec{b}·\vec{c})\vec{a} \) and \( \vec{a}×(\vec{b}×\vec{c})=(\vec{a}·\vec{c})\vec{b}−(\vec{a}·\vec{b})\vec{c} \).
2. Equating gives \( (\vec{a}·\vec{b})\vec{c}−(\vec{b}·\vec{c})\vec{a}=\vec0 \).
3. But \( (\vec{a}×\vec{c})×\vec{b}=(\vec{a}·\vec{b})\vec{c}−(\vec{c}·\vec{b})\vec{a} \), which is exactly this expression, so the condition is \( (\vec{a}×\vec{c})×\vec{b}=\vec0 \).
Teacher's Note:
1. Expand both sides and compare, then recognise the remaining expression as another triple product.
2. The vector triple product is not associative in general.
(a) \( \vec{c} \)
(b) \( \vec{a}×\vec{b} \)
(c) Both \( \vec{c} \) and \( \vec{a}×\vec{b} \)
(d) \( \vec{b} \) and \( \vec{c} \)
Show Answer & Explanation
Answer: (c) Both \( \vec{c} \) and \( \vec{a}×\vec{b} \)
Explanation:
1. A cross product is perpendicular to both of its factors.
2. The factors of \( (\vec{a}×\vec{b})×\vec{c} \) are \( \vec{a}×\vec{b} \) and \( \vec{c} \).
3. So it is perpendicular to both of them.
Teacher's Note:
1. Read the outermost cross product to see which two vectors the result is perpendicular to.
2. The result lies in the plane of \( \vec{a} \) and \( \vec{b} \).
(a) \( 3\vec{a} \)
(b) \( 2\vec{a} \)
(c) \( \vec{a} \)
(d) \( \vec0 \)
Show Answer & Explanation
Answer: (b) \( 2\vec{a} \)
Explanation:
1. \( \hat{i}×(\vec{a}×\hat{i})=(\hat{i}·\hat{i})\vec{a}−(\hat{i}·\vec{a})\hat{i}=\vec{a}−a_1\hat{i} \).
2. Sum over the three unit vectors: \( 3\vec{a}−(a_1\hat{i}+a_2\hat{j}+a_3\hat{k})=3\vec{a}−\vec{a} \).
3. The sum equals \( 2\vec{a} \).
Teacher's Note:
1. This is a standard result: summing over the three axes gives twice the vector.
2. Expand each term with the triple product formula.
(a) 1
(b) 24
(c) 36
(d) 4
Show Answer & Explanation
Answer: (d) 4
Explanation:
1. Use \( (\vec{a}×\vec{b})·(\vec{c}×\vec{d})=(\vec{a}·\vec{c})(\vec{b}·\vec{d})−(\vec{a}·\vec{d})(\vec{b}·\vec{c}) \).
2. \( \vec{a}·\vec{c}=4, \vec{b}·\vec{d}=−1+(−2)+4=1, \vec{a}·\vec{d}=2−3+1=0 \).
3. So the value is \( 4×1−0=4 \).
Teacher's Note:
1. The scalar product of two cross products is a 2 × 2 determinant of dot products.
2. Compute the four dot products carefully.
(a) \( |\vec{a}|^2 \)
(b) \( |\vec{b}|^2 \)
(c) \( |\vec{c}|^2 \)
(d) 0
Show Answer & Explanation
Answer: (b) \( |\vec{b}|^2 \)
Explanation:
1. \( (\vec{a}×\vec{b})·(\vec{c}×\vec{b})=(\vec{a}·\vec{c})(\vec{b}·\vec{b})−(\vec{a}·\vec{b})(\vec{b}·\vec{c}) \).
2. Adding \( (\vec{a}·\vec{b})(\vec{b}·\vec{c}) \) gives \( |\vec{b}|^2(\vec{a}·\vec{c}) \).
3. Comparing with \( λ(\vec{a}·\vec{c}) \) gives \( λ=|\vec{b}|^2 \).
Teacher's Note:
1. Apply the Lagrange-type identity for the dot product of two cross products.
2. The terms with \( \vec{a}·\vec{b} \) cancel.
(a) \( \vec{a}·\vec{b} \)
(b) \( 3(\vec{a}·\vec{b}) \)
(c) 0
(d) \( 2(\vec{a}·\vec{b}) \)
Show Answer & Explanation
Answer: (d) \( 2(\vec{a}·\vec{b}) \)
Explanation:
1. \( (\vec{a}×\hat{i})·(\vec{b}×\hat{i})=(\vec{a}·\vec{b})(\hat{i}·\hat{i})−(\vec{a}·\hat{i})(\hat{i}·\vec{b})=\vec{a}·\vec{b}−a_1b_1 \).
2. Adding the three terms: \( 3(\vec{a}·\vec{b})−(a_1b_1+a_2b_2+a_3b_3) \).
3. This equals \( 2(\vec{a}·\vec{b}) \).
Teacher's Note:
1. Use the same four-vector identity for each axis vector.
2. The leftover sum of products is the dot product itself.
(a) \( |\vec{a}|^2(\vec{b}·\vec{c}) \)
(b) \( |\vec{b}|^2(\vec{a}·\vec{c}) \)
(c) \( |\vec{c}|^2(\vec{a}·\vec{b}) \)
(d) 0
Show Answer & Explanation
Answer: (a) \( |\vec{a}|^2(\vec{b}·\vec{c}) \)
Explanation:
1. \( (\vec{a}×\vec{b})·(\vec{a}×\vec{c})=|\vec{a}|^2(\vec{b}·\vec{c})−(\vec{a}·\vec{b})(\vec{a}·\vec{c}) \).
2. Since \( \vec{a} \) is perpendicular to both \( \vec{b} \) and \( \vec{c} \) (being parallel to \( \vec{b}×\vec{c} \)), \( \vec{a}·\vec{b}=\vec{a}·\vec{c}=0 \).
3. Hence the value is \( |\vec{a}|^2(\vec{b}·\vec{c}) \).
Teacher's Note:
1. A vector parallel to \( \vec{b}×\vec{c} \) is perpendicular to both \( \vec{b} \) and \( \vec{c} \).
2. That kills the second term of the identity.
(a) 1
(b) 2
(c) 4
(d) 0
Show Answer & Explanation
Answer: (c) 4
Explanation:
1. \( [\vec{a}\ \vec{b}\ \vec{a}×\vec{b}]=(\vec{a}×\vec{b})·(\vec{a}×\vec{b}) \) (the triple product is cyclic).
2. This equals \( |\vec{a}×\vec{b}|^2=4 \).
Teacher's Note:
1. Rotate the scalar triple product so that the cross product comes first.
2. A vector dotted with itself gives the square of its magnitude.
(a) \( 24(\hat{i}+\hat{j}−2\hat{k}) \)
(b) \( 24(\hat{i}−\hat{j}−\hat{k}) \)
(c) \( 12(2\hat{i}+\hat{j}−3\hat{k}) \)
(d) \( 12(\hat{i}−2\hat{j}+3\hat{k}) \)
Show Answer & Explanation
Answer: (a) \( 24(\hat{i}+\hat{j}−2\hat{k}) \)
Explanation:
1. \( \vec{a}×\vec{b}=(1−6,\ 9−2,\ 4−3)=(−5,7,1) \) and \( \vec{c}×\vec{d}=(1+8,\ −4+1,\ 2+1)=(9,−3,3) \).
2. \( (−5,7,1)×(9,−3,3)=(21+3,\ 9+15,\ 15−63)=(24,24,−48) \).
3. This equals \( 24(\hat{i}+\hat{j}−2\hat{k}) \).
Teacher's Note:
1. Find the two cross products separately and then cross them.
2. Factor out the common number to match the option.
(a) \( [\vec{a}\ \vec{b}\ \vec{c}]\vec{d} \)
(b) \( [\vec{b}\ \vec{c}\ \vec{d}]\vec{a} \)
(c) \( [\vec{c}\ \vec{d}\ \vec{a}]\vec{b} \)
(d) The null vector
Show Answer & Explanation
Answer: (d) The null vector
Explanation:
1. For coplanar vectors, \( \vec{a}×\vec{b} \) and \( \vec{c}×\vec{d} \) are both perpendicular to the same plane.
2. So they are parallel and their cross product is zero.
3. The answer is the null vector.
Teacher's Note:
1. Two cross products of vectors lying in one plane are both normal to that plane.
2. Parallel vectors have a zero cross product.
(a) 2
(b) 7
(c) 9
(d) 11
Show Answer & Explanation
Answer: (c) 9
Explanation:
1. \( (\vec{b}×\vec{c})×(\vec{c}×\vec{a})=[\vec{a}\ \vec{b}\ \vec{c}]\vec{c} \), so \( [\vec{a}\ \vec{b}\ \vec{c}]=3 \).
2. \( [\vec{b}×\vec{c}\ \vec{c}×\vec{a}\ \vec{a}×\vec{b}]=[\vec{a}\ \vec{b}\ \vec{c}]^2 \).
3. The value is \( 3^2=9 \).
Teacher's Note:
1. Memorise: the scalar triple product of the three cross products is the square of \( [\vec{a}\ \vec{b}\ \vec{c}] \).
2. The given condition gives \( [\vec{a}\ \vec{b}\ \vec{c}] \) directly.
(a) \( \hat{i}−\hat{j}+\hat{k} \)
(b) \( 2\hat{i}−2\hat{j} \)
(c) \( 3\hat{i}−\hat{j}+\hat{k} \)
(d) \( 2\hat{i}+2\hat{j}−\hat{k} \)
Show Answer & Explanation
Answer: (b) \( 2\hat{i}−2\hat{j} \)
Explanation:
1. \( \vec{a}·\vec{c}=1−1+1=1 \) and \( \vec{a}·\vec{b}=1−1−1=−1 \).
2. \( \vec{a}×(\vec{b}×\vec{c})=(\vec{a}·\vec{c})\vec{b}−(\vec{a}·\vec{b})\vec{c}=\vec{b}+\vec{c} \).
3. \( \vec{b}+\vec{c}=2\hat{i}−2\hat{j} \).
Teacher's Note:
1. Use the expansion \( \vec{a}×(\vec{b}×\vec{c})=(\vec{a}·\vec{c})\vec{b}−(\vec{a}·\vec{b})\vec{c} \) and substitute the components.
2. Take care with the signs of the dot products.
(a) −4
(b) 4
(c) 2
(d) −2
Show Answer & Explanation
Answer: (a) −4
Explanation:
1. \( \vec{a}·\vec{c}=1−6+6=1 \) and \( \vec{a}·\vec{b}=2−2+3=3 \).
2. \( \vec{a}×(\vec{b}×\vec{c})=\vec{b}−3\vec{c}=(2−3,\ 1−9,\ −1+6)=(−1,−8,5) \).
3. \( p+q+r=−1−8+5=−4 \).
Teacher's Note:
1. Use the expansion \( \vec{a}×(\vec{b}×\vec{c})=(\vec{a}·\vec{c})\vec{b}−(\vec{a}·\vec{b})\vec{c} \) and substitute the components.
2. Add the components only at the very end.
(a) 2
(b) 4
(c) 0
(d) 3
Show Answer & Explanation
Answer: (c) 0
Explanation:
1. \( \vec{p}·\vec{r}=4−10+6=0 \) and \( \vec{p}·\vec{q}=6−10+4=0 \).
2. \( \vec{p}×(\vec{q}×\vec{r})=(\vec{p}·\vec{r})\vec{q}−(\vec{p}·\vec{q})\vec{r}=\vec0 \).
3. So the magnitude is 0.
Teacher's Note:
1. Check the dot products before computing any cross product; here both vanish.
2. A quick check saves a long calculation.
(a) \( \hat{i} \)
(b) \( \hat{j} \)
(c) \( \hat{k} \)
(d) The null vector
Show Answer & Explanation
Answer: (d) The null vector
Explanation:
1. Here \( \hat{j}×\hat{k}=\hat{i} \), so \( \hat{i}×\hat{i}=\vec0 \).
2. Similarly \( \hat{k}×\hat{i}=\hat{j} \) gives \( \hat{j}×\hat{j}=\vec0 \) and \( \hat{i}×\hat{j}=\hat{k} \) gives \( \hat{k}×\hat{k}=\vec0 \).
3. The sum is the null vector.
Teacher's Note:
1. Evaluate the brackets first using the cyclic rule \( \hat{i}×\hat{j}=\hat{k} \).
2. Each term becomes the cross product of a vector with itself.
(a) Perpendicular
(b) Parallel
(c) Inclined at \( \pi/3 \)
(d) Inclined at \( \pi/6 \)
Show Answer & Explanation
Answer: (b) Parallel
Explanation:
1. Expanding: \( (\vec{a}·\vec{c})\vec{b}−(\vec{b}·\vec{c})\vec{a}=(\vec{a}·\vec{c})\vec{b}−(\vec{a}·\vec{b})\vec{c} \).
2. So \( (\vec{a}·\vec{b})\vec{c}=(\vec{b}·\vec{c})\vec{a} \).
3. Since both scalars are non-zero, \( \vec{c} \) is a scalar multiple of \( \vec{a} \), i.e. they are parallel.
Teacher's Note:
1. Cancel the common term and read off the proportionality.
2. The conditions \( \vec{a}·\vec{b}≠0 \), \( \vec{b}·\vec{c}≠0 \) ensure the multiples are non-zero.
(a) Coplanar with \( \vec{b} \) and \( \vec{c} \) and parallel to \( \vec{a} \)
(b) Coplanar with \( \vec{a} \) and \( \vec{b} \), parallel to \( \vec{c} \)
(c) Coplanar with \( \vec{b} \) and \( \vec{c} \), and orthogonal to \( \vec{a} \)
(d) Coplanar with \( \vec{a} \) and \( \vec{b} \), and orthogonal to \( \vec{c} \)
Show Answer & Explanation
Answer: (c) Coplanar with \( \vec{b} \) and \( \vec{c} \), and orthogonal to \( \vec{a} \)
Explanation:
1. \( \vec{a}×(\vec{b}×\vec{c})=(\vec{a}·\vec{c})\vec{b}−(\vec{a}·\vec{b})\vec{c} \) is a combination of \( \vec{b} \) and \( \vec{c} \), hence coplanar with them.
2. It is a cross product with \( \vec{a} \) as a factor, so it is perpendicular to \( \vec{a} \).
Teacher's Note:
1. The triple product lies in the plane of the two vectors inside the bracket.
2. It is perpendicular to the vector outside the bracket.
(a) \( 2\vec{a} \)
(b) \( −2\vec{a} \)
(c) \( \vec{a} \)
(d) \( −\vec{a} \)
Show Answer & Explanation
Answer: (b) \( −2\vec{a} \)
Explanation:
1. \( (\vec{a}×\hat{i})×\hat{i}=−\hat{i}×(\vec{a}×\hat{i}) \).
2. The sum is therefore \( −\sum \hat{i}×(\vec{a}×\hat{i})=−2\vec{a} \).
Teacher's Note:
1. Reverse the order of the outer cross product to reuse the standard sum.
2. The sign flips.
(a) 1
(b) 0
(c) −2
(d) −1
Show Answer & Explanation
Answer: (b) 0
Explanation:
1. \( (\vec{a}×\vec{b})·(\vec{c}×\vec{d})=(\vec{a}·\vec{c})(\vec{b}·\vec{d})−(\vec{a}·\vec{d})(\vec{b}·\vec{c}) \).
2. Directly, \( \vec{a}×\vec{b}=(−2,2,0) \) and \( \vec{c}×\vec{d}=(2,2,0) \).
3. Their dot product is \( −4+4+0=0 \), which agrees with the identity \( 1·1−1·1=0 \).
Teacher's Note:
1. Either use the four-vector identity or compute the two cross products.
2. Both give the same result.
(a) 1
(b) 0
(c) −2
(d) −1
Show Answer & Explanation
Answer: (d) −1
Explanation:
1. The identity states \( (\vec{a}×\vec{b})·(\vec{c}×\vec{d})=(\vec{a}·\vec{c})(\vec{b}·\vec{d})−(\vec{a}·\vec{d})(\vec{b}·\vec{c}) \).
2. Comparing, \( K=−1 \).
Teacher's Note:
1. Remember the determinant form with rows \( \vec{a}·\vec{c}, \vec{a}·\vec{d} \) and \( \vec{b}·\vec{c}, \vec{b}·\vec{d} \).
2. The cross term carries the minus sign.
(a) 0
(b) 1
(c) 2
(d) −1
Show Answer & Explanation
Answer: (a) 0
Explanation:
1. Write each term as a 2 × 2 determinant of dot products.
2. \( (\vec{b}·\vec{a})(\vec{c}·\vec{d})−(\vec{b}·\vec{d})(\vec{c}·\vec{a}) \) + \( (\vec{c}·\vec{b})(\vec{a}·\vec{d})−(\vec{c}·\vec{d})(\vec{a}·\vec{b}) \) + \( (\vec{a}·\vec{c})(\vec{b}·\vec{d})−(\vec{a}·\vec{d})(\vec{b}·\vec{c}) \).
3. All six products cancel in pairs, so the sum is 0.
Teacher's Note:
1. Expand every term with the four-vector identity.
2. Cancellation of all six terms is the whole proof.
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